Light modulator, light source using the light modulator, display apparatus using the light modulator, and method for driving the light modulator

ABSTRACT

A light modulator is comprised of two unit devices each using surface plasmon generated at the interface between thin metal films respectively formed on prisms and an electro-optical material, and a mirror. Both of the transmitted light due to absorption and re-radiation, and the reflected light arising from the unit devices are made into the outgoing light, the incident light on the next unit device, or the incident light on the mirror. Consequently, all light beams can be utilized as the final outgoing light beams with no loss of light. Further, the color of light can be spatially divided, and still further, it can also be temporally divided by changing the wavelength due to a voltage. As a result, the original light can be divided both temporally and spatially with almost no loss by combining two unit devices so configured as to re-radiate the absorbed light by surface plasmon using surface plasmon and a mirror, and thus utilizing both of the reflected light and the transmitted light.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a light modulator. More particularly,it relates to a light modulator utilizing surface plasmon, a lightsource and a display apparatus using the light modulator, and a methodfor driving the light modulator.

2. Description of the Related Art

As a conventional display apparatus, especially, a field sequentialdisplay apparatus, there is disclosed an apparatus using a color filterdisk (eg., “Color Liquid Crystal Display” written and edited by ShunsukeKobayashi: published in Dec. 14, 1990, P.117) With this apparatus, acolor filter disc colored in red, green, and blue, i.e., three primarycolors of light is placed in front of a monochrome cathode ray tube, androtates in synchronism with display to enable color display. Similarly,color display is also possible even by placing the color filter disc infront of a white light source, and combining a black shutter(black-and-white shutter type display device) therewith.

Further, as an apparatus of another system, on pages 120 and 121 of theaforesaid document “Color Liquid Crystal Display”, there is shown anapparatus for performing field sequential color display by combining twohigh-speed liquid crystal display devices referred to as π cells, and atotal of three sheet polarizers and color sheet polarizers in front of amonochrome CRT(cathode ray tube).

Further, there is also shown the technology using a CRT, LED (lightemitting diode), or cold cathode fluorescent tube as a backlight, andusing a liquid crystal display as a black shutter on pages 122 and 123in the document “Color Liquid Crystal Display”. With this apparatus,backlights of respective three primary colors are prepared so as toalternately flash. One example thereof is shown as a field sequentialfull color LCD in “Monthly Published Display”, the July issue, pp.11-16,(1998). In this example, the cold cathode fluorescence tube backlightwhich is illumination light of commonly used liquid crystal displayapparatus is temporally switched among red, green, and blue.

In recent years, there are proposed a light modulator utilizing anelectromagnetic wave supported by the interface between a metal and aninsulator (a dielectric material) referred to as a surface plasmon wave(SPW), a display apparatus which permits color display by utilizing thislight modulator, and a light source thereof as a display apparatuswhereby color display is implemented without using the foregoing colorfilter and color light source. That is, conductors such as metals can bedefined as a gas of electrons in electrostatic equilibrium inside acontinuum of positive fixed charges. It can be considered as a“condensed” electron plasma with electron density approximately equal to10²³ electrons per cm³. There exists a longitudinal wave referred to asa surface plasma oscillation in addition to a volume plasma oscillationwhich is a normal plasma oscillation. The electric field due to thesurface plasma oscillation has a periodic wave form in a directionparallel to the metal surface, while having a form of evanescent wavewhich evanesces exponentially in a direction perpendicular to the metalsurface. Plasmons are quanta associated with the plasma oscillation(collective wave excitation of a conductive electronic gas) in themetal. Because of high electron density, quantum effects dominate. Thesurface plasmon waves can be optically excited by resonant coupling. Thecondition for resonance is strongly dependent on the refractive indicesand thickness of the media near the metal-insulator interface. Theintensity of the light wave can be modulated by coupling the light wavewith the surface plasmon wave. Generally, if coupling between thesurface plasmon wave and the light wave is strong, the attenuation ofthe emitted light wave is strong, and if coupling is weak, there occursalmost no attenuation of the emitted light wave.

Attenuated total reflection (ATR) effect has been utilized to opticallyexcite surface plasmon waves through a high-index prism. Light,traveling in free-space, is sent toward the metal-insulator interfacethrough the prism with an angle larger than the critical angle,producing an evanescent wave field which may overlap the surface plasmonwave field. If the propagation constant Kev of the evanescent wave is inharmony with the propagation constant Ksp of the surface plasmon, thesurface plasmon resonance is excited on the metal surface. Twoconfigurations are mainly used for optically exciting the surfaceplasmon wave. The first is Otto's ATR configuration. This Otto'sconfiguration is shown in FIG. 1A. In this Otto's configuration, thereexists a small air gap between a metal medium layer 101 stacked on athick insulator 102 and a high-index prism 103. A surface plasmon wave105 is optically excited by the incident light. Further, the secondconfiguration used to optically excite surface plasmon waves isKretschmann's modified ATR configuration as shown in FIG. 1B. In thisconfiguration, a thin metallic foil 101 is inserted between the prism103 and the insulator 102. Surface plasmon waves 105 are also opticallyexcited by absorbed light which will not be reflected light 106. Thisconfiguration is more practical since there is no air gap. It is notedthat the high-index prism 103 for generating the evanescent wave may bea diffraction grating with a period smaller than the wavelength of theincident light, or other optical components.

Here, when a prism is used as an optical component, the propagationconstant (wave number) Kev of the evanescent wave is represented by thefollowing equation (1): $\begin{matrix}\begin{matrix}{K_{ev} = {{{n(\omega)} \cdot {K_{0}(\omega)} \cdot \sin}\quad \theta}} \\{= {{{n(\omega)} \cdot {\omega/c} \cdot \sin}\quad \theta}} \\{= {{{n(\lambda)} \cdot 2}{{\pi/\lambda} \cdot \sin}\quad \theta}}\end{matrix} & (1)\end{matrix}$

where c is the speed of light in vacuum, ω is the angular frequency, λis the wavelength, n(ω) and n(λ) are the refractive indices of the prismin the case of an angular frequency ω and a wavelength λ, respectively,K₀(ω) is the wave number in the case of an angular frequency ω) invacuum, and θ is the incident angle of light with respect to theunderside of the prism. Therefore, the wave number of the evanescentwaves can be harmonized with the propagation constant of the metalsurface plasmon by adjusting the refractive index n(ω) or n(λ) of theprism and the incident angle θ of light.

On the other hand, the propagation constant Ksp of the surface plasmonis given by the following equation 2, where the angular frequency of thesurface plasmon is ω, and the dielectric indices of the metal and thedielectric indices of the low-index medium in contact with the metal arerespectively ∈m and ∈0, $\begin{matrix}\begin{matrix}{k_{sp} = {\frac{\omega}{c} \cdot \sqrt{\frac{{ɛ_{m}(\omega)} \cdot ɛ_{0}}{{ɛ_{m}(\omega)} + ɛ_{0}}}}} \\{= {\frac{2\pi}{\lambda} \cdot \sqrt{\frac{{ɛ_{m}(\lambda)} \cdot ɛ_{0}}{{ɛ_{m}(\lambda)} + ɛ_{0}}}}}\end{matrix} & (2)\end{matrix}$

where the ∈m(ω) and ∈0(ω) are the dielectric indices of the metal in thecase of the angular frequency ω and the wavelength λ, respectively.Here, since the ∈m is a complex number, the propagation constant Ksp isalso a complex number. The evanescent waves generated by using a prismwhen Kev=Ksp generates the surface plasmon. In order to strongly excitethe metal surface plasmon, the metal surface plasmon itself must be awave with a long life. That is, it is required that the imaginary partof the propagation constant Ksp is small, and the attenuation associatedwith propagation is small.

The imaginary part of the propagation constant Ksp is approximativelysolved, assuming that respective complex numbers are Ksp=Ksp′+iKsp″, and∈m=∈m′+i∈m″ (the ∈to be precise, depends on the angular frequency or thewavelength), yielding the following expression 3: $\begin{matrix}\begin{matrix}{k_{sp}^{''} \approx \quad {{\frac{\omega}{c} \cdot ( \frac{{ɛ_{m}(\omega)}^{\prime} \cdot ɛ_{0}}{{ɛ_{m}(\omega)}^{\prime} + ɛ_{0}} )^{3R}} \times \frac{{ɛ_{m}(\omega)}^{''}}{2( {ɛ_{m}(\omega)}^{\prime} )^{2}}}} \\{\approx \quad {{\frac{2\pi}{\lambda} \cdot ( \frac{{ɛ_{m}(\lambda)}^{\prime} \cdot ɛ_{0}}{{ɛ_{m}(\lambda)}^{\prime} + ɛ_{0}} )^{3R}} \times \frac{{ɛ_{m}(\lambda)}^{''}}{2( {ɛ_{m}(\lambda)}^{\prime} )^{2}}}}\end{matrix} & (3)\end{matrix}$

Therefore, the factor which decides the intensity of the metal surfaceplasmon is ∈m″/(∈m′)₂ (the ∈, to be precise, depends on the angularfrequency or the wavelength), and the metal to excite the metal surfaceplasmon is desirably a metal whose value of |∈m″/(∈m′)₂| is small.Specifically, silver (Ag), gold (Au), copper (Cu), aluminum (Al) and thelike are usable.

There are proposed a liquid crystal display device (U.S. Pat. No.5,451,980), and a projector (U.S. Pat. No. 5,570,139), each of whichselects a wavelength based on an electric field using a material whoserefractive index varies with the application of electric field such as aliquid crystal as a low-index dielectric to perform display utilizingsurface plasmon. The example of the publication of the device in theacademic meeting is shown in “Appl. Phys. Lett.”, U.S., 1995, vol. 67,the 19 th number, pp. 2759 to 2761. In this reference, as shown in FIG.2A, there is illustrated a device whereby the absorption wavelength ismade variable, and the wavelength region of the reflected light iselectrically changed using a liquid crystal. Further, FIG. 2B shows themeasurements (a broken curve) and the calculated results (solid curve)of the characteristics of the reflected light intensity with respect towavelengths when the voltage value in the aforesaid device is varied. Inthe device, a 60° SF₆ glass prism is used as a prism 103, and a 50-nmsilver thin film is evaporated thereon as a thin metal film 101. A 50-nmMgF₂ layer is then evaporated at a 50° oblique angle onto the silverfilm as an alignment layer 108. A substrate 110 is so configured thatthe same alignment layer 108 is obliquely evaporated on an ITO filmwhich is a transparent electrode formed on a glass substrate. A 4-μmcell gap is ensured by spacers 109, and then filled with BL009manufactured by Merck KGaA as a liquid crystal 107. As shown in FIG. 2A,a white light is incident on the device through a sheet polarizer as ap- and linearly polarized light, and a voltage is applied thereto todetermine the dependence of the reflected light on the wavelength. Theresults are shown in FIG. 2B. At a voltage of 0 V, there is anabsorption maximum in the vicinity of 640 nm. The absorption maximumshifts towards the lower wavelengths with the application of a voltage.At 10V, it is at 560 nm, and at 30 V, it is at 450 nm. The measuredresults are in good agreement with the calculated results.

Further, as another technology, there is a technology utilizingre-radiation of the absorbed light. As the example thereof, adescription will be given to the technology shown in “SID 97 DIGEST”U.S., 1997, pp. 63-66. FIG. 3A is a cross sectional view of a device forobtaining transmitted light in a specific wavelength range byimplementing the conventional Kretschmann method in a symmetricstructure. FIG. 3B is a diagram showing the calculated results of thetransmitted light intensity with respect to the wavelength when therefractive index of the central medium is changed in the device. Thisdevice is considered the same as the one obtained by removing thesubstrate 110 side, and providing a structure identical with the upperside structure on the lower side in symmetric relation in the devicehaving the structure shown in FIG. 2A. However, the film thickness ofthe electro-optical material 111 of the central part is set much thinneras compared with the device of FIG. 2A. This symmetric structure and thevery thin central electro-optical material 111 enable the coupling ofthe surface plasmon wave generated at the interface on the incident sideto the surface plasmon wave at the next interface with the metal togenerate another surface plasmon wave on the outgoing side. This surfaceplasmon wave re-radiates the light with the same wavelength. In thismanner, it is possible to re-radiate the absorbed light. FIG. 3B showstheoretical calculated results when the anisotropic refractive index dnof the central material is changed from 0 to: 0.2, and 0.5 in thisdevice. When the dn is 0, the device radiates the light of a wavelengthof 450 nm, at 0.2 and 0.5, 530-nm light and 650-nm light are radiated,respectively. Since surface plasmon is a surface effect, the filmthickness of the central material is set to be very thin, or about onewavelength in order to effect such re-radiation. When a liquid crystalmaterial is used as the central material, it is considered that theresponse speed can be about two orders of magnitude faster than theresponse speed of a conventional liquid crystal device because of thethinness of the film thickness.

Furthermore, as still other technology of the reference, the technologyas shown in FIG. 4 shows an example of the configuration of adirect-view type liquid crystal display apparatus for performing a fieldsequential display utilizing surface plasmon. Here, one device of FIG.3A is used as a device 100. The light from a line source 112 is incidentthrough a cylindrical lens 113 on the device 100, and one color of thethree primary colors of light is selected for every time period. Thelight is applied onto the whole surface of a liquid crystal panel 115 bya reflector 114 having a stepped surface to permit field sequentialdisplay. Further, in patent publications or other references, there areproposed other liquid crystal display devices or projectors utilizingthem. As the technology described in U.S. Pat. No. 5,570,139, an exampleof a light source for a liquid crystal display device utilizing surfaceplasmon as shown in FIG. 5 will be described. White light is appliedfrom the upper right to be sequentially incident on a plurality of(three) unit devices 100A, 100B, and 100C. Thus, the outgoing lighttherefrom is established itself as a light source. At respective unitdevices 100A, 100B, and 100C, light beams of specific wavelength ranges,i.e., blue, green, and red light beams are individually absorbed toobtain respective colors of yellow, magenta, and cyan. This cycle isrepeated in three devices to obtain a light of a prescribed color.

On the other hand, as an example in which surface plasmon is utilizedfor a projector, there is a technology shown in “SPIE”, vol.3019, pp.35-40 (1997). FIG. 6 is a cross sectional view of an example of theprojector utilizing surface plasmon according to the technology. Acentral surface plasmon device 100D has almost the same structure as theone shown in FIG. 5, except that the prisms 103 of FIG. 5 are integratedinto one unit. There are placed a lamp 116, a reflector 117, a relaylens 118, an integrator 119, and a sheet polarizer 120 on the incidentside. On the other hand, there is placed a reflection type liquidcrystal display apparatus or the like, not shown, which performsmonochrome modulation through a projection lens 121 to obtain an imageon the outgoing side, thus performing image display. The light from thelamp is collected in one direction by the reflector, and then broughtclose to a parallel beam in a narrow region by the relay lens and theintegrator. The light beam is then aligned into either polarized lightby the sheet polarizer, and selection of color and image display areperformed at the surface plasmon device. Finally, the image is projectedthrough the projection lens. The projection can be accomplished based onthe field sequential display.

Further, in Japanese Laid-open Patent Publication No. Hei 5-313108,there is disclosed a light modulator in which a metal-insulatorinterface is formed adjacent to a planar wave guide for carrying a lightwave. With the light modulator, a high frequency voltage applied to theinterface causes the insulator to resonate, generating a surface plasmonwave on the interface. The resulting wave is coupled to a graduallyvanishing light wave in the wave guide, thus changing the intensity ofthe light wave.

The foregoing prior-art light modulator, especially, the light modulatorutilizing surface plasmon, and a display apparatus utilizing the same,encounter the following problems. The first problem lies in that thestructure is complicated. This is attributable to the fact that, in theprior art, three unit devices each having a wavelength variable by anelectric field are required for simultaneously obtaining light beams ofthree primary colors of specific wavelength ranges. The second problemlies in that loss of light is high. The reason for this is that only thereflected light from which light at surface plasmon has been absorbed,or the re-radiated light of the absorbed light is utilized. Therefore,the whole of light which has not been used results in a loss. Forexample, with the technology of FIG. 4, the period during which onecolor produced by the field sequential display is displayed, other 2colors of the three primary colors are not utilized at all. The thirdproblem lies in that there exists no light modulator capable of ensuringa division both temporally and spatially.

SUMMARY OF THE INVENTION

It is therefore an object of the present invention to provide a lightmodulator with a simplified structure. It is another object of thepresent invention to provide a light modulator whereby the loss of lightis minimized. It is a still further object of the present invention toprovide a light modulator capable of ensuring division both temporallyand spatially. It is yet further object of the present invention toprovide a display apparatus using the aforementioned light modulator,and a display method thereof.

The present invention relates to a light modulator utilizing surfaceplasmon generated at the interface between a thin metal film and anelectro-optical material. Then, the present invention is characterizedby including two unit devices, and a mirror, the two unit devices, eachcomprising: a pair of prisms individually provided with thin metal filmsat their respective undersides, and the thin metal films beingoppositely disposed, and an electro-optical material sandwiched betweenthe oppositely disposed thin metal films, wherein the two unit devicesare disposed in parallel to each other such that respective one surfacesof the one prisms of the unit devices are in contact with each other soas to ensure the arrangement of the thin metal films in parallelrelation to each other, and the mirror is disposed such that the mirrorside thereof faces a direction in parallel to the thin metal films, andextends along the top of the prism of one unit device on the sidethereof not in contact with another unit device. As the electro-opticalmaterial, a liquid crystal material is used. Alternatively, an air gapcan be adopted in place of the electro-optical material. The thicknessof the air gap may also be changed by a piezo material provided betweenthe prisms constituting the unit device. Further, it is possible toadopt a diffraction grating in place of the prism. Furthermore, a lightsource can be configured, or a liquid crystal display apparatus or aliquid crystal projector can be configured, by utilizing the foregoinglight modulator.

With the light modulator according to the present invention, all of theincident light can be utilized in the final outgoing light with no lossby making both of the transmitted light due to absorption andre-radiation generated by the unit device and the reflected light intothe outgoing light; the light incident on the next unit device, or thelight incident on the mirror. Further, the color of light can bespatially divided. Still further, it can also be divided temporally bychanging the wavelength by a voltage.

BRIEF DESCRIPTION OF THE DRAWINGS

FIGS. 1A and 1B are illustrative diagrams of a conventional surfaceplasmon wave generator by Otto and a surface plasmon wave generator byKretschmann in the prior art, respectively.

FIGS. 2A and 2B are, respectively, a cross sectional view of aconfiguration of a device whereby the absorption wavelength is madevariable by using a conventional liquid crystal and the wavelength rangeof the reflected light is electrically changed, and a graph showing themeasured and calculated results of the reflected light intensitycharacteristics with respect to the wavelength when the voltage value ischanged in this device.

FIGS. 3A and 3B are, respectively, a cross sectional view of a deviceimplementing the conventional Kretschmann method in a symmetricstructure to obtain the transmitted light within a specific wavelengthrange; and a graph showing the calculated results of the transmittedlight intensity with respect to the wavelength when the refractive indexof the central material is changed in this device.

FIG. 4 is a view of the configuration of a direct-view type liquidcrystal display apparatus for performing the field sequential displayutilizing a conventional surface plasmon.

FIG. 5 is a view showing an example of a light source for a conventionalliquid crystal display device utilizing surface plasmon.

FIG. 6 is a view of the configuration of one example of a conventionalprojector utilizing surface plasmon.

FIGS. 7A and 7B are views illustrating the configuration and theoperation of the first embodiment of the present invention,respectively.

FIGS. 8A through 8C are views illustrating the configuration and theoperation of the third embodiment of the present invention.

FIGS. 9A through 9C are views illustrating the configuration and theoperation of the fourth embodiment of the present invention.

FIG. 10 is a view showing the configuration of the fifth embodiment ofthe present invention.

FIG. 11 is a view showing the configuration of the sixth embodiment ofthe present invention.

FIGS. 12A and 12B are graphs showing the characteristic example of afilter and the spectral characteristic in the sixth embodiment of thepresent invention.

FIG. 13 is a graph showing a driving method in the seventh embodiment ofthe present invention.

FIGS. 14A and 14B are graphs showing the spectral characteristic in theeighth embodiment of the present invention.

FIGS. 15A through 15C are views showing the operation of the ninthembodiment of the present invention.

FIGS. 16A and 16B are graphs showing the intensity of spatially dividedlight of the eleventh embodiment of the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Below, the preferred embodiments of the present invention will bedescribed in detail by reference to the appended drawings.

First, a first embodiment of the present invention will be described. Asshown in FIG. 7A, the apparatus of the first embodiment of the presentinvention comprises first and second unit devices 1 and 2 eachimplementing the Kretschmann method in a symmetric structure, and onemirror 3. If required, a device for aligning the polarization directioninto one direction is added thereto. Here, a polarization conversiondevice 4 is provided in a light incident path. The first and second unitdevices 1 and 2 each implementing the Kretschmann method in a symmetricstructure are so configured that the respective inclined surfaces of twoprisms 11 and 12 each having a right triangle cross section areoppositely disposed, and thin metal films 13 and 14 are respectivelyformed on the inclined surfaces, and further an electro-optical material15 whose refractive index varies in accordance with the electric fieldstrength is inserted between the oppositely disposed thin metal films 13and 14. Then, the first and second unit devices 1 and 2 are arranged inparallel relation to each other with respective one surfaces of theprisms substantially in contact with each other. As a result, eachunderside of the prisms 11 and 12 and the thin metal films 13 and 14 arearranged in parallel relation to one another. At the same time, thesurface side of the mirror 3 is also disposed so that it is parallel tothe aforesaid parallel plane, and one end thereof is substantially incontact with the top of the prism of the second unit device 2 on theside thereof not in contact with the first unit device 1. Further, thepolarization conversion device 4 is disposed at the incident light sideposition of the first unit device 1 not in contact with the mirror 3,i.e., at the position opposing the side of the prism 12 not in contactwith the second unit device 2.

FIG. 7B is a diagram illustrating the operation of the apparatus of thefirst embodiment thus configured. It is a diagram schematically showinghow the light beams of three primary colors of R, G, and B (red, green,and blue) are transmitted. The white light which has been made into alinearly polarized light by the polarization conversion device 4 isincident on one surface of the prism 12 of the first unit device 1., andreaches the thin metal film 14. Here, at a certain time, the first unitdevice 1 on the incident side absorbs a light of red, and re-radiatesit. Therefore, red light is emitted. The reflected light including theother green and blue light is incident on the second unit device 2. Atthe second unit device 2, the light reaches the thin metal film 13through the prism 11, and blue light is absorbed, and re-radiated.Therefore, green light is emitted as reflected light. Further, bluelight passes through the second unit device 2, and then it is reflectedby the mirror 3, and emitted therefrom. Thus, white light is spatiallydivided in the order of red, green, and blue. Further, the refractiveindex of the electro-optical material 15 is changed by individuallyapplying the first unit device 1 and the second unit device 2 with avoltage. Therefore it is possible to change the wavelength of the lightto be absorbed and re-radiated. For example, in the case where green andred are absorbed and re-radiated at the first unit device 1 and thesecond unit device 2, respectively, the white light is spatially dividedin the order of green, blue, and red. The spatially divided light canalso be divided temporally by performing a temporal switching in thismanner. The loss of light is also very low. Especially insertion of thepolarization conversion device 4 for aligning non-polarized light withlinearly polarized light at the incident side results in almost no lossof light.

Then, a second embodiment of the present invention will be described. Inthe second embodiment of the present invention, a liquid crystalmaterial is used as the electro-optical material 15 whose refractiveindex varies with the electric field of the first embodiment. In thiscase, there is formed an alignment layer for aligning the liquid crystalmaterial, if required. The operation of the second embodiment is thesame as that of the first embodiment. The liquid crystal alignment ofthe liquid crystal material serving as the electro-optical material 15is changed by the application of a voltage, and the refractive index ofthe liquid crystal material changes due to the anisotropic refractiveindex which the liquid crystal has. Consequently, it is possible tochange the wavelength by a voltage. Especially noteworthy is thefollowing fact. Since the liquid crystal material region is a very thinfilm with a thickness of about one wavelength, switching is done notbased on a bulk, but based on only the surface. Accordingly, theresponse can be obtained about two orders of magnitude faster than thedevice using a conventional liquid crystal material. Consequently, alight modulator capable of giving a fast response can be obtained.

For example, referring to FIG. 7, prisms of 60° SF₆ glass (manufacturedby Shott Co., Germany) are used as the prisms 11 and 12 of the first andsecond unit devices 1 and 2, and silver thin films are evaporatedthereon as the thin metal films 13 and 14. Further, MgF₂ is obliquelyevaporated thereon as an alignment layer, which is not shown. A liquidcrystal is sandwiched as the electro-optical material 15 between theprisms 11 and 12. Thus, the prisms 11 and 12 are joined together withoutusing an adhesive. The thin metal films 13 and 14 are wired so as toenable the application with a voltage. The first and second unit devices1 and 2 are each thus configured and are optically cemented to eachother using a matching oil with a refractive index of 1.805, almost thesame as that of SF₆. Further, a mirror 3 is placed. The light from awhite light source is shined thereon through a sheet polarizer servingas the polarization conversion device 4. Then, the light is spatiallydivided into red, green, and blue by applying a voltage across thewiring, i.e., between the thin metal films 13 and 14. Further, it ispossible to perform temporal switching by adjusting the voltage value.It is possible to provide high-speed switching in the order of (1) red,green, and blue, (2) green, blue, and red, and (3) blue, red, and green.

In this case, the one of the rutile crystal structure obtained byheating titanium oxide is used as the prism 11 or 12. The refractiveindex is found to be about 2.8. The first and second unit devices 1 and2 are manufactured using the prisms, and arranged in parallel relationto each other. Then, a mirror 3 is further provided thereon. There isalso provided a polarization conversion device 4 for convertingnon-polarized light into p-polarized light. With such a configuration,the efficiency is enhanced by the effects of the polarization conversiondevice and the use of the high-index prisms much more than with theforegoing configuration. Further, although a consideration was alsogiven to the case where the FDS1 glass of HOYA Co., with a refractiveindex of about 1.92 was used, the efficiency of the rutile prism wasfound to be higher.

Then, a third embodiment of the present invention will be described. Inthe third embodiment of the present invention, an air gap is adopted inplace of the material 15 whose refractive index varies with the electricfield of the first embodiment, and the material exhibiting thepiezoelectric effect is placed at either end or both ends of the spacebetween the opposing prisms 11 and 12. FIG. 8A is a diagram showing theconfiguration of the third embodiment. Piezo materials 16 arerespectively disposed on both ends of the space between the prisms 11and 12 in place of the electro-optical material 15 provided in the firstembodiment, and thus, an air gap 17 is provided between the prisms 11and 12 by the piezo materials 16.

FIGS. 8B and 8C are diagrams illustrating the operation of the thirdembodiment. In this third embodiment, as distinct from the first andsecond embodiments, the application of a voltage changes not therefractive index, but the thickness of the air gap 17. The applicationof the piezo materials 16 with a voltage causes distortion due to thevoltage value. As a result, the elongation as shown FIG. 8B, orshrinkage as shown in FIG. 8C occurs, thereby making it possible tochange the thickness of the air gap 17. The coupling conditions forsurface plasmon are changed by utilizing this property to obtain thesame effects as in the first and second embodiments. The advantage ofthis method is that, since the region of the air gap 17 has a lowerrefractive index than a liquid crystal as compared with the case wherethe liquid crystal is used, the prisms 11 and 12 are not required tohave high refractive indices. This is advantageous for achieving a lowercost.

Specific example of the third embodiment include the use of zinc oxide(ZnO) in terms of easiness for achieving a thinner film as the materialhaving the piezoelectric effect. The device of this embodiment can bemanufactured in the same manner as in the second embodiment, except thatthe liquid crystal is not used, and the following process for using thepiezo material. Thin films 16 of zinc oxide are formed and patterned onboth ends of the silver thin film 13 on each prism 11 of the unitdevices 1 and 2. Then, a silver paste is applied thereon in a very smallamount by means of a control type dispenser to be joined together withthe side of the prism 12 on which the silver thin film 14 is formed.Thus, the air gap 17 is formed between respective silver thin films 13and 14 of the prisms 11 and 12 by the zinc oxide thin film 16. It isnoted that the mirror 3 and the polarization conversion device 4 areused. This specific example can provide the same high efficiency as inthe specific example of the first embodiment. Further, in the thirdembodiment, zinc oxide is used as the piezo material, but any materialcan be employed as long as they can be formed into thinner films. Forexample, even with aluminum nitride (AlN), a good thin film can beformed by a magnetron sputtering method or a dual beam sputteringmethod. Alternatively, with zinc oxide, a better thin film can beobtained by an ECR plasma sputtering method. On the other hand, athinner film can also be achieved with a PZT system in recent years.

Then, a fourth embodiment of the present invention will be described. Inthe fourth embodiment of the present invention, there is used thematerial exhibiting the piezoelectric effect in the same manner as inthe third embodiment. However, as shown in FIG. 9A, only an air gap 17is provided in place of the electro-optical material 15 in the firstembodiment. Materials 16 exhibiting the piezoelectric effect arerespectively placed on the surfaces of the respective prisms 11 and 12of the unit devices 1 and 2 through which light of incidence,transmission, reflection, or the like will not. pass. In this fourthembodiment, the thickness of the air gap is varied in the same manner asin the third embodiment. The application of the piezo materials 16 witha voltage causes distortion due to the voltage value. As a result, theelongation as shown FIG. 9B, or shrinkage as shown in FIG. 9C occurs,thereby making it possible to change the thickness of the air gap 17between the prisms 11 and 12. The advantages of this method are asfollows. In addition to the advantage of the third embodiment, the piezomaterial 16 is not required to be formed into a thin film, and whendisposed on the whole surface of each prism as shown in FIGS. 9A, 9B,and 9C, the patterning accuracy is not required because patterning isnot necessary, resulting in a low manufacturing cost. Further, theelectrode for the piezo material 16 is easy to extract. It is notedthat, since the direction of elongation and shrinkage of the piezomaterial 16 differs from the opposing direction between the prisms 11and 12, a slight side-to-side movement of the figure occurs, but itoccurs in a very narrow range, and hence it can be ignored. Further, inthis fourth embodiment, although the same material as in the thirdembodiment can be used as the piezo material 16, such a reduction inthickness of the film as in the third embodiment is not required in thisembodiment. Therefore, more various piezo materials can be used.

Then, a fifth embodiment of the present invention will be described. Inthe fifth embodiment of the present invention, diffraction gratings areused in place of the prisms 11 and 12 of the first through fourthembodiments. As shown in FIG. 10, a diffraction grating 18 is used ateach portion on which the prism of the first embodiment was placed. Thatis, thin metal films 13 and 14 are respectively formed on both surfacesof the electro-optical material 15 with a desired thickness. Thediffraction gratings 18 are individually disposed on their respectivesurfaces of the thin metal films 13 and 14. For the diffraction grating18, a diffraction grating having a shorter period than the wavelength ofincident light is selected. In this embodiment, in accordance with thefirst through fourth embodiments, either the electro-optical materialsuch as a liquid crystal or the material exhibiting the piezoelectriceffect may be used. In this fifth embodiment, the same operation as inthe first embodiment is possible, as well as a particularly large prismis not required. As a result, the whole apparatus becomes compact insize, and a reduction in weight can also be achieved.

Then, the sixth embodiment of the present invention will be described.In the sixth embodiment, a filter is disposed at the outgoing side ofthe second unit device used in the first through fifth embodiments. FIG.11 shows the configuration adapted to the first embodiment as the sixthembodiment. A filter 19 for improving wavelength characteristics isdisposed at the outgoing side of the second unit device 2. The filter 19has characteristics that compensate for differences in wavelength rangeand intensity between the outgoing light which has been absorbed andre-radiated at each unit device and the outgoing light which hasundergone only absorption, and has been reflected at the unit device 1and the unit device 2. The characteristics of the filter 19 are, ifrequired, also the characteristics for cutting the wavelength regionwherein absorption will not satisfactorily arise from the surfaceplasmon absorption under the conditions such as the voltage, filmthickness, and refractive index to be used. FIG. 12A shows one exampleof the characteristics of the filter used in this sixth embodiment. Thecharacteristics are of the absorption and re-radiation close to thecharacteristics shown in FIG. 8B. It is indicated that thecharacteristics are for cutting the light within the unnecessarywavelength region included in the light reflected from the second unitdevice when the light modulator having peaks at wavelengths of 460 nm,550 nm, and 680 nm. FIG. 12B shows the wavelength characteristics of theoutgoing light in each unit space spatially divided when the sixthembodiment is implemented. It shows the case where red light and bluelight is absorbed and re-radiated at the first unit device 1 and thesecond unit device 2, respectively, and green light is reflected fromthe second unit device 2. It is indicated that the unnecessarywavelength region is cut so that the spatial division of colors issatisfactorily achieved.

Then, a seventh embodiment of the present invention will be described.This seventh embodiment relates to a method for applying an electricfield, i.e., a driving method in the first through sixth embodiments.FIG. 13 shows one example of the driving method in the seventhembodiment. This example of the driving method is characterized in thatit is for not setting constant the wavelength of the light absorbedwithin the field sequential sub-field time, but shifting it as shown inthe figure. That is, the amplitude of the voltage to be applied withinthe sub-field is changed. FIG. 14A is a graph showing the wavelengthcharacteristic range to be shifted by the driving method. FIG. 14B is agraph showing a difference in wavelength characteristics between thecase where the aforesaid driving method is utilized (solid curve) andthe case where it is not utilized (a broken curve). With this drivingmethod, since the amplitude of the voltage to be applied within thesub-field time is varied, the emitted light corresponds to the timeaverage of the one which has shifted its wavelength characteristics inaccordance with the change. Therefore, it is possible to adjust thewidth of the wavelength region. At the same time, the wavelength regionof the light reflected from the second unit device can also be adjusted.In FIG. 14B, although a positive and negative symmetrical voltage is tobe applied on the liquid crystal portion, application of a voltage ofonly either polarity is sufficient when problems such as imagepersistence will not occur. Even in the case of the piezo material, theconditions for the applied voltage value differs therefrom, but theimplementation is possible in the same manner.

Then, an eighth embodiment of the present invention will be described.In the eighth embodiment of the present invention, a compression colordivision light source is configured by using one light modulator of thefirst through seventh embodiments. Although not particularly shown inthis embodiment, in the first through seventh embodiments, since therespective first and second unit devices 1 and 2 are capable of dividinglight into light beams of different wavelengths, and respectivelyemitting them therefrom, it is possible to configure the compressioncolor division light source. Here, the compression color division lightsource denotes a source of both temporally and spatially divided light,and having a low loss of light. For example, as shown in FIG. 13B, itcan be implemented by a combination of a white light source includinglight beams of a large number of wavelength regions, or the like, andthe light modulator of the first embodiment. Similarly, it can beimplemented by a combination of the white light source, or the like, andany one light modulator of the second through seventh embodiments. Thelight source of this eighth embodiment eliminates a loss of light in thefield sequential display.

Then, a ninth embodiment of the present invention will be described. Inthe ninth embodiment of the present invention, a liquid crystal displayapparatus of the field sequential method is configured by using any onelight modulator of the first through seventh embodiments, or thecompression color division light source of the eighth embodiment. FIGS.15A through 15C are views illustrating a part of the liquid crystaldisplay apparatus according to the ninth embodiment; and the operationthereof. That is, a liquid crystal 20 of the liquid crystal displayapparatus is configured as a liquid crystal panel of a direct-view type,reflection type, or projection type. One micro lens 23 is disposedopposite to every set of three aperture portions 22 out of the apertureportions individually defined by the respective light-shielding portions21 of the liquid crystal 20. Any one light modulator or light source ofthe first through eighth embodiments is placed at the left-hand portionoutside the figure with respect to each micro lens 23. With thisconfiguration, the optical path of light of each divided color isadjusted by the lens, and the light is to be incident from the left sideof the figure. The light enters the liquid crystal layer through eachmicro lens, and passes through a picture element structure from theaperture portions and the light shielding portions. In a first period,as shown in FIG. 15A, red, blue, and green are sequentially displayed ontheir respective pixels, vertically from the highest one. In the nextperiod, green, red, and blue are displayed in this order as shown inFIG. 15B, and in the final period, blue, green, and red are displayed inthis order as shown in FIG. 15C. Repetition of this procedure permitsthe field sequential display by a method whereby colors are switchedindividually on each picture element. Consequently, a liquid crystaldisplay apparatus with a low loss of light can be obtained.

Then, a tenth embodiment of the present invention will be described. Inthis tenth embodiment, a projector is configured based on the firstthrough ninth embodiments. Although not shown, this embodiment isimplemented by adapting the first through ninth embodiments to a part ofthe projector apparatus. The operation thereof is the same as describedabove. The projection type such as a projector shows a high loss oflight, and hence requires the high intensity of the light source. Thus,it has presented problems of an increase in dissipation power, areduction in size of the apparatus, and the like. With the configurationof this embodiment, a projector with no loss of light can be obtained.Further, as the display method with the projector, there are methodsusing other various apparatuses such as a DMD (digital mirror device)and a TMA (thin film micro-mirror array), other than the method usingthe liquid crystal display apparatus of the ninth embodiment. Further,the embodiment using a large number of these devices is also possible.

Then, an eleventh embodiment of the present invention will be described.The eleventh embodiment of the present invention relates to a method fordriving the liquid crystal display apparatus in the ninth embodiment, orthe projector of in the tenth embodiment. The light beams which havebeen spatially divided and emitted have different intensities for everyunit space. This is attributable to the designing conditions andmanufacturing conditions of the unit device, differences in reflectanceof the mirror, and optical path difference, and the medium in theoptical path, and the like other than the difference in intensitybetween the light emitted due to the absorption and re-radiation, andthe light emitted due to only twice absorption and reflection. Then, theliquid crystal display apparatus or the projector is driven so as tocorrect the differences by an apparatus for monochrome modulation, orthe like to be used therein.

FIGS. 16A and 16B are graphs showing the operation of the eleventhembodiment. FIG. 16A shows the intensity of each spatially divided lightbeam obtained by the light modulator. FIG. 16B shows the range in whichthe intensity of the monochrome modulation for the characteristics ofFIG. 16A is set. The one resulting from the synergistic effect betweenthe characteristics of FIGS. 16A and 16B can be obtained as an actualdisplay. This method can eliminate the difference in intensity generatedby the light modulator.

As described above, according to the present invention, the lightmodulator is comprised of two unit devices utilizing the surface plasmongenerated at the interface between the thin metal film and theelectro-optical material, and a mirror. Both of the transmitted lightdue to absorption and re-radiation, and the reflected light generated bythe unit device are made into the outgoing light, the incident light onthe next unit device, or the incident light on the mirror. Consequently,all light beams can be utilized as the final outgoing light beams withno loss of light. Further, the color of light can be spatially divided,and still further, it can also be temporally divided by changing thewavelength due to a voltage.

Therefore, according to the present invention, there can be provided thefollowing effects. First, since only two unit devices to be applied withan electric field is required, the structure becomes very simple.Secondly, since both the transmitted light which has been re-coupled bya symmetrical structure and the reflected light are used artfully andeffectively, the light can be utilized effectively with a very low lossof light. Thirdly, since the light can be spatially divided intorespective wavelength regions due to the device structure, while it canalso be temporally divided because of the variance of the wavelength dueto the application of an electric field, there can be provided a lightmodulator capable of performing a division both temporally andspatially. Fourthly, since the refractive index is lowered because ofthe simplified structure of the apparatus and use of the piezoelectriceffect, costly prisms or costly diffraction gratings become unnecessary,and cheap prisms or cheap diffraction gratings can be used. Therefore,the apparatus can be implemented at a low cost. Fifthly, since thediffraction grating is used in place of the prisms, the whole apparatusbecomes compact in size, and is reduced in weight. Sixthly, since thefilter for correcting the wavelength characteristics is used, and thewavelength characteristics are improved by devising the driving method,the wavelength characteristics of the emitted light are enhanced.

What is claimed is:
 1. A light modulator using surface plasmon generatedat the interface between a thin metal film and an electro-opticalmaterial, comprising two unit devices and a mirror, wherein said twounit devices, each comprising a pair of prisms individually providedwith thin metal films at their respective undersides, and said thinmetal films being oppositely disposed, and an electro-optical materialbeing sandwiched between said oppositely disposed thin metal films, andsaid two unit devices are disposed in parallel to each other such thatrespective one surfaces of the one prisms of said unit devices are incontact with each other so as to ensure the arrangement of said thinmetal films in parallel relation to each other, and said mirror isdisposed such that the mirror side thereof faces the direction inparallel to said thin metal films, and extends along the top of theprism of one unit device on the side thereof not in contact with anotherunit device.
 2. The light modulator according to claim 1, wherein aliquid crystal material is used as said electro-optical material.
 3. Thelight modulator according to claim 1, wherein said prism is replacedwith a diffraction grating.
 4. The light modulator according to claim 1wherein a device for aligning the polarization direction into onedirection is disposed on the incident light side of the other unitdevice not in contact with said mirror.
 5. The light modulator accordingto claim 1, wherein a filter for adjusting the wavelengthcharacteristics is disposed on the outgoing side of said one unitdevice.
 6. A light source of a compression color division system,comprising a combination of said light modulator according to claim 1and a source of white light to be incident on said light modulator.
 7. Adisplay apparatus comprising: a light source according to claim 6, whichilluminates a liquid crystal panel, and a display unit to display theprojected image on said liquid crystal panel or a screen.
 8. A displayapparatus comprising: a light modulator according to claim 1, whichilluminates a liquid crystal panel, and a display unit to display theprojected image on said liquid crystal panel or a screen.
 9. A methodfor driving a light modulator of the type using surface plasmongenerated at the interface between a thin metal film and anelectro-optical material, comprising two unit devices and a mirror,wherein said two unit devices, each comprising a pair of prismsindividually provided with thin metal films at their respectiveundersides, and said thin metal films being oppositely disposed, and anelectro-optical material being sandwiched between said oppositelydisposed thin metal films, and said two unit devices are disposed inparallel to each other such that respective surfaces of the individualprisms of said unit devices are in contact with each other so as toensure the arrangement of said thin metal film in parallel relation toeach other, and said mirror is disposed such that the mirror sidethereof faces the direction in parallel to said thin metal films andextends along the top of the prism of one unit device on the sidethereof not in contact with another unit device, comprising the steps ofspatially dividing the incident light into light beams of plurality ofwavelengths, and changing the voltage to be applied on said thin metalfilms.
 10. A method for driving a display apparatus of the typecomprising a light modulation using surface plasmon generated at theinterface between a thin metal film and an electro-optical material,comprising two unit devices and a mirror, wherein said two unit devices,each comprising a pair of prisms individually provided with thin metalfilms at their respective undersides, and said thin metal films beingoppositely disposed, and an electro-optical material being sandwichedbetween said oppositely disposed thin metal films, and said two unitdevices are disposed in parallel to each other such that respectivesurfaces of the individual prisms of said unit devices are in contactwith each other so as to ensure the arrangement of said thin metal filmsin parallel relation to each other, and said mirror is disposed suchthat the mirror side thereof faces the direction in parallel to saidthin metal films, and extends along the top of the prism of one unitdevice on the side thereof not in contact with another unit device,comprising driving said display apparatus so as to correct a differencein intensity of optical power on spatial division due to said lightmodulator.
 11. A method for driving a display apparatus comprising acombination of a light modulator of the type using surface plasmongenerated at the interface between a thin metal film and anelectro-optical material, comprising two unit devices and a mirror,wherein said two unit devices, each comprising a pair of prismsindividually provided with thin metal films at their respectiveundersides, and said thin metal films being oppositely disposed, and anelectro-optical material being sandwiched between said oppositelydisposed thin metal films, and said two unit devices are disposed inparallel to each other such that respective surfaces of the individualprisms of said unit devices are in contact with each other so as toensure the arrangement of said thin metal films in parallel relation toeach other, and said mirror is disposed such that the mirror sidethereof faces the direction in parallel to said thin metal films, andextends along the top of the prism of one unit device on the sidethereof not in contact with another unit device, and a source of whitelight to be incident on said light modulator, comprising driving saiddisplay apparatus so as to correct a difference in intensity of opticalpower on spatial division due to said light modulator.